Added topics: depend on time/rate - Skipped

Size: px
Start display at page:

Download "Added topics: depend on time/rate - Skipped"

Transcription

1 VIa- 1 Added topics: depend on time/rate - Skipped a) diffusion rate material moves in medium faster motion more friction affect equilibrium separations like electrophoresis HPLC pharmacological cross blood-brain barrier drug absorption b) charge transfer many reactions are redox move charge in enzyme -- special method-- Marcus theory also move charge in cell through Na + or K + channel signaling, neurobiology, muscle activation, etc. c) Photobiology transfer of energy after excitation light absorption and re-emission (fluorescence) structural changes, energetics, signaling Single molecule enzymology It is popular now to try to study single molecules as they undergo some process, enzyme reaction is a good one We discuss average data for many molecules in sample How differ if look at 1 molecule, enzyme turns over can follow rate of individual steps Idea fluorescent enzyme, changes with substrate Trap enzyme so dilute yet not move, add substrate Signal will stay on various times, depending on turnover

2 VIa- 2 Cholesterol oxidase, S=cholesterol, P=oxidized cholest. Active site has flavin adenine dinucleotide (FAD) catalyse oxidation with O 2 E FAD + S k-1 k 1 E FAD S k 2 k -2 E FADH 2 + P O 2 Observe on/off signal for varying amount of time Plot number of times within t t+δt histogram Results the various enzyme molecules fit MM but had different rates, could be due to different conformers from Tinoco

3 VIa- 3 Photobiology: We will return to basics of absorption and fluorescence at end of course in the spectroscopy section idea: light consists of photons E=hν=hc/λ where ν frequency of light, λ wavelength transmitted energy: I t = I 0 (10) -εbc - intensity is flux: cm -2 s -1 b path in cm, c concentration (molar), ε - absorptivity amount absorbed is then: I abs = I 0 (1-(10) -εbc ) note: (10) -εbc =e -2.3εbc if c is low = [A], then I abs ~I 0 (2.3)εb[A] e -x = 1-x+x 2 /2-... excitation rate: r = d[a]/dt = I abs 1000/b from:1/b~cm -1 & 1000cm 3 /L = I 0 (2303)εb[A]/ b integrate rate: [A] = [A 0 ]exp[-i 0 (2303)εt] - 1 st order Jablonski diagram, like a kinetic mechanism, follow energy Engel p , alternate view, kinetic analogy Table 26.1

4 VIa- 4 Quenching provide alternate energy path, like parallel mech. reduce fluorescence view as yield: I f 0 /I f = 1 + (k q /k f )[Q] - Stern-Volmer plot: I f 0 /I f vs [Q] Lifetime: 1/τ f = k f + k q [Q] Diffusion Engel Chap 24, Tinoco, Chapter 6 Analysis of gas collisions will yield the gas law PV = η R T = N/N 0 R T but in form: PV = 1/3 N m u 2 mean velocity since Kinetic Energy ~ 1/2 m υ 2 ~ 1/2 m u 2 PV = 2/3 n (N 0 1/2 m u 2 ) m u 2 =3k B T PV=nRT ½ T measure average Kinetic Energy RT = 2/3 U tr average trans energy [in solution and big molecules also vibration and rotation] [ collisions relate to translations] temperature average kinetic energy Distribution of energies relate to Probability of any one E i, discrete E i Boltzmann: P j = N j /N = g j e -E j/kt /Σ i g i e -E i/kt each weight by e -E i/kt Maxwell-Boltzmann velocity distribution continuous dp(u) = F(u)du = 4π (m/2πkt) 3/2 u 2 e -mu 2/2kT

5 VIa- 5 can be used to describe collisions and other properties of gases Liquids Diffusion better model J x flow of concentration through area Fick 1st J x = -D (dc/dx) - need concentration gradient if dc/dx constant flow Fick 2 nd ( c/ t) = D ( 2 c/ x 2 ) time dependent gradient vary w/x D determine experimentally from Fick s law (cm 2 s -1 ) relates to distributions: D = x 2 /2t x displacement from initial position reverse time to travel distribution (average) D = k B T/ƒ where ƒ frictional coefficient (Einstein) ƒ = 6π η r η viscosity, r radius (assume spherical) could measure size from D shape means measure ƒ greater than calc ƒ 0 ƒ/ƒ 0 increase: non-sherical, or bind solvent

6 VIa- 6 Sedimentation diffuse in medium gravity drive can be molecule or cellular component (big) gravity bouyant force keep up (velocity depend) F = mg m V 2 ρ g ƒυ = m υ/ t : friction slows ρ = density of medium, V 2 = partial specific vol. Centrifuge increase g gravity acceleration effect = a a = ω 2 x ω frequency, x distribution from center terminal velocity becomes: U t = m(1 V 2 ρ) ω 2 x /ƒ sedimentation coefficient: s = U t /ω 2 x = m(1 V 2 ρ)/ƒ combine with diffusion ƒ = kt/d Mass: M = RTs/D(1 V 2 ρ) in molecular weight Electrophoresis charge molecules move in field u = ZeE/f u/e electrophoretic mobility D diffusion constant small molecule ~10-5 cm 2 s -1 large molecule smaller/slower H ion can hop in water Shows up in pre-exponential M + N k d k -d (M N)* P A d = 4π r MN (D M + D N ) N 0 /1000 N 0 Avogadro & (1000 cm 3 L) r MN encounter distance ~ few Å ~ L mol -1 s -1 for r ~ 4 x 10-8 cm, D ~ 1.5 x 10-5 cm 2 s -1 max rate if E a ~ 0 See Tinoco Table 7.5 / pg. 374 typical rates ions can be faster big molecule slower / even with enzyme

BAE 820 Physical Principles of Environmental Systems

BAE 820 Physical Principles of Environmental Systems BAE 820 Physical Principles of Environmental Systems Estimation of diffusion Coefficient Dr. Zifei Liu Diffusion mass transfer Diffusion mass transfer refers to mass in transit due to a species concentration

More information

v AB + C à AC + B Ø Bonds breaking

v AB + C à AC + B Ø Bonds breaking Chemistry Study Guide 3 v Kinetics reaction rates Ø Catalyst Ø Temperature Ø Concentration Ø Bonds Ø Surface area v Kinetics Ø Kinetic energy is directly proportional to the temperature Ø Gasses will react

More information

Chapter 14. The Ideal Gas Law and Kinetic Theory

Chapter 14. The Ideal Gas Law and Kinetic Theory Chapter 14 The Ideal Gas Law and Kinetic Theory 14.1 Molecular Mass, the Mole, and Avogadro s Number To facilitate comparison of the mass of one atom with another, a mass scale know as the atomic mass

More information

What the Einstein Relations Tell Us

What the Einstein Relations Tell Us What the Einstein Relations Tell Us 1. The rate of spontaneous emission A21 is proportional to υ 3. At higher frequencies A21 >> B(υ) and all emission is spontaneous. A 21 = 8π hν3 c 3 B(ν) 2. Although

More information

Part I.

Part I. Part I bblee@unimp . Introduction to Mass Transfer and Diffusion 2. Molecular Diffusion in Gasses 3. Molecular Diffusion in Liquids Part I 4. Molecular Diffusion in Biological Solutions and Gels 5. Molecular

More information

XV 74. Flouorescence-Polarization-Circular-Dichroism- Jablonski diagram Where does the energy go?

XV 74. Flouorescence-Polarization-Circular-Dichroism- Jablonski diagram Where does the energy go? XV 74 Flouorescence-Polarization-Circular-Dichroism- Jablonski diagram Where does the energy go? 1) Excite system through A Absorbance S 0 S n Excite from ground excited singlet S = 0 could be any of them

More information

Physics 1501 Lecture 35

Physics 1501 Lecture 35 Physics 1501: Lecture 35 Todays Agenda Announcements Homework #11 (Dec. 2) and #12 (Dec. 9): 2 lowest dropped Honors students: see me after the class! Todays topics Chap.16: Temperature and Heat» Latent

More information

Kinetic Model of Gases

Kinetic Model of Gases Kinetic Model of Gases Section 1.3 of Atkins, 6th Ed, 24.1 of Atkins, 7th Ed. 21.1 of Atkins, 8th Ed., and 20.1 of Atkins, 9th Ed. Basic Assumptions Molecular Speeds RMS Speed Maxwell Distribution of Speeds

More information

PHOTOCHEMISTRY NOTES - 1 -

PHOTOCHEMISTRY NOTES - 1 - - 1 - PHOTOCHEMISTRY NOTES 1 st Law (Grotthus-Draper Law) Only absorbed radiation produces chemical change. Exception inelastic scattering of X- or γ-rays (electronic Raman effect). 2 nd Law (Star-Einstein

More information

Lecture 10. Lidar Effective Cross-Section vs. Convolution

Lecture 10. Lidar Effective Cross-Section vs. Convolution Lecture 10. Lidar Effective Cross-Section vs. Convolution q Introduction q Convolution in Lineshape Determination -- Voigt Lineshape (Lorentzian Gaussian) q Effective Cross Section for Single Isotope --

More information

2. Molecules in Motion

2. Molecules in Motion 2. Molecules in Motion Kinetic Theory of Gases (microscopic viewpoint) assumptions (1) particles of mass m and diameter d; ceaseless random motion (2) dilute gas: d λ, λ = mean free path = average distance

More information

Reaction Dynamics (2) Can we predict the rate of reactions?

Reaction Dynamics (2) Can we predict the rate of reactions? Reaction Dynamics (2) Can we predict the rate of reactions? Reactions in Liquid Solutions Solvent is NOT a reactant Reactive encounters in solution A reaction occurs if 1. The reactant molecules (A, B)

More information

CD Basis Set of Spectra that is used is that derived from comparing the spectra of globular proteins whose secondary structures are known from X-ray

CD Basis Set of Spectra that is used is that derived from comparing the spectra of globular proteins whose secondary structures are known from X-ray CD Basis Set of Spectra that is used is that derived from comparing the spectra of globular proteins whose secondary structures are known from X-ray crystallography An example of the use of CD Modeling

More information

CHEM Atomic and Molecular Spectroscopy

CHEM Atomic and Molecular Spectroscopy CHEM 21112 Atomic and Molecular Spectroscopy References: 1. Fundamentals of Molecular Spectroscopy by C.N. Banwell 2. Physical Chemistry by P.W. Atkins Dr. Sujeewa De Silva Sub topics Light and matter

More information

19-9 Adiabatic Expansion of an Ideal Gas

19-9 Adiabatic Expansion of an Ideal Gas 19-9 Adiabatic Expansion of an Ideal Gas Learning Objectives 19.44 On a p-v diagram, sketch an adiabatic expansion (or contraction) and identify that there is no heat exchange Q with the environment. 19.45

More information

K20: Temperature, Heat, and How Heat Moves

K20: Temperature, Heat, and How Heat Moves K20: Temperature, Heat, and How Heat Moves Definition of Temperature Definition of Heat How heat flows (Note: For all discussions here, particle means a particle of mass which moves as a unit. It could

More information

Rate of Heating and Cooling

Rate of Heating and Cooling Rate of Heating and Cooling 35 T [ o C] Example: Heating and cooling of Water E 30 Cooling S 25 Heating exponential decay 20 0 100 200 300 400 t [sec] Newton s Law of Cooling T S > T E : System S cools

More information

Biophysics I. DIFFUSION

Biophysics I. DIFFUSION Biophysics I. DIFFUSION Experiment add a droplet of ink to a glass of water Observation: the stain spreads and eventually colours the entire fluid add a droplet of ink to HOT and COLD water Observation:

More information

Fluorescence (Notes 16)

Fluorescence (Notes 16) Fluorescence - 2014 (Notes 16) XV 74 Jablonski diagram Where does the energy go? Can be viewed like multistep kinetic pathway 1) Excite system through A Absorbance S 0 S n Excite from ground excited singlet

More information

Chapter 18. Fundamentals of Spectrophotometry. Properties of Light

Chapter 18. Fundamentals of Spectrophotometry. Properties of Light Chapter 18 Fundamentals of Spectrophotometry Properties of Light Electromagnetic Radiation energy radiated in the form of a WAVE caused by an electric field interacting with a magnetic field result of

More information

Rate of change of velocity. a=dv/dt. Acceleration is a vector quantity.

Rate of change of velocity. a=dv/dt. Acceleration is a vector quantity. 9.7 CENTRIFUGATION The centrifuge is a widely used instrument in clinical laboratories for the separation of components. Various quantities are used for the description and the calculation of the separation

More information

Rotational Brownian motion; Fluorescence correlation spectroscpy; Photobleaching and FRET. David A. Case Rutgers, Spring 2009

Rotational Brownian motion; Fluorescence correlation spectroscpy; Photobleaching and FRET. David A. Case Rutgers, Spring 2009 Rotational Brownian motion; Fluorescence correlation spectroscpy; Photobleaching and FRET David A. Case Rutgers, Spring 2009 Techniques based on rotational motion What we studied last time probed translational

More information

Measuring the size and shape of macromolecules. Hydrodynamics: study of the objects in water How do the move? Translation Rotation

Measuring the size and shape of macromolecules. Hydrodynamics: study of the objects in water How do the move? Translation Rotation Measuring the size and shape of macromolecules Hydrodynamics: study of the objects in water How do the move? Translation Rotation 1) Movement with no external forcefree diffusion 2) Movement under the

More information

C C C C 2 C 2 C 2 C + u + v + (w + w P ) = D t x y z X. (1a) y 2 + D Z. z 2

C C C C 2 C 2 C 2 C + u + v + (w + w P ) = D t x y z X. (1a) y 2 + D Z. z 2 This chapter provides an introduction to the transport of particles that are either more dense (e.g. mineral sediment) or less dense (e.g. bubbles) than the fluid. A method of estimating the settling velocity

More information

Electron temperature is the temperature that describes, through Maxwell's law, the kinetic energy distribution of the free electrons.

Electron temperature is the temperature that describes, through Maxwell's law, the kinetic energy distribution of the free electrons. 10.3.1.1 Excitation and radiation of spectra 10.3.1.1.1 Plasmas A plasma of the type occurring in spectrochemical radiation sources may be described as a gas which is at least partly ionized and contains

More information

Stellar Structure. Observationally, we can determine: Can we explain all these observations?

Stellar Structure. Observationally, we can determine: Can we explain all these observations? Stellar Structure Observationally, we can determine: Flux Mass Distance Luminosity Temperature Radius Spectral Type Composition Can we explain all these observations? Stellar Structure Plan: Use our general

More information

collisions of electrons. In semiconductor, in certain temperature ranges the conductivity increases rapidly by increasing temperature

collisions of electrons. In semiconductor, in certain temperature ranges the conductivity increases rapidly by increasing temperature 1.9. Temperature Dependence of Semiconductor Conductivity Such dependence is one most important in semiconductor. In metals, Conductivity decreases by increasing temperature due to greater frequency of

More information

1. Transition dipole moment

1. Transition dipole moment 1. Transition dipole moment You have measured absorption spectra of aqueous (n=1.33) solutions of two different chromophores (A and B). The concentrations of the solutions were the same. The absorption

More information

Chapter 8: Introduction to Atomic Spectrometry

Chapter 8: Introduction to Atomic Spectrometry Chapter 8: Introduction to Atomic Spectrometry Read: pp. 215 228 Problems: 2,4,5,6,9 Why choose atomic spectrometry? Three major types of spectrometric methods for identifying elements present in matter:

More information

ε tran ε tran = nrt = 2 3 N ε tran = 2 3 nn A ε tran nn A nr ε tran = 2 N A i.e. T = R ε tran = 2

ε tran ε tran = nrt = 2 3 N ε tran = 2 3 nn A ε tran nn A nr ε tran = 2 N A i.e. T = R ε tran = 2 F1 (a) Since the ideal gas equation of state is PV = nrt, we can equate the right-hand sides of both these equations (i.e. with PV = 2 3 N ε tran )and write: nrt = 2 3 N ε tran = 2 3 nn A ε tran i.e. T

More information

Oxidation & Reduction II. Suggested reading: Chapter 5

Oxidation & Reduction II. Suggested reading: Chapter 5 Lecture 1 Oxidation & Reduction II Suggested reading: Chapter 5 Recall from Last time: Redox Potentials The Nernst equation: E cell E 0 RT F ln Q Cell Potential and ph For the H + /H couple at 1 bar and

More information

Similarities and differences:

Similarities and differences: How does the system reach equilibrium? I./9 Chemical equilibrium I./ Equilibrium electrochemistry III./ Molecules in motion physical processes, non-reactive systems III./5-7 Reaction rate, mechanism, molecular

More information

How DLS Works: Interference of Light

How DLS Works: Interference of Light Static light scattering vs. Dynamic light scattering Static light scattering measures time-average intensities (mean square fluctuations) molecular weight radius of gyration second virial coefficient Dynamic

More information

Chemistry 795T. Lecture 7. Electromagnetic Spectrum Black body Radiation. NC State University

Chemistry 795T. Lecture 7. Electromagnetic Spectrum Black body Radiation. NC State University Chemistry 795T Lecture 7 Electromagnetic Spectrum Black body Radiation NC State University Black body Radiation An ideal emitter of radiation is called a black body. Observation: that peak of the energy

More information

Chemistry 795T. Black body Radiation. The wavelength and the frequency. The electromagnetic spectrum. Lecture 7

Chemistry 795T. Black body Radiation. The wavelength and the frequency. The electromagnetic spectrum. Lecture 7 Chemistry 795T Lecture 7 Electromagnetic Spectrum Black body Radiation NC State University Black body Radiation An ideal emitter of radiation is called a black body. Observation: that peak of the energy

More information

Chemistry 471 Final exam 12/18/06 Page 1 of 6 Name:

Chemistry 471 Final exam 12/18/06 Page 1 of 6 Name: Chemistry 47 Final exam /8/6 Page of 6 Please leave the exam pages stapled together. The formulas are on a separate sheet. This exam has 5 questions. You must answer at least 4 of the questions. You may

More information

CHAPTER 19 Molecules in Motion. 1. Matter transport is driven by concentration gradient.

CHAPTER 19 Molecules in Motion. 1. Matter transport is driven by concentration gradient. CHAPTER 19 Molecules in Motion I. Transport in Gases. A. Fick s Law of Diffusion. 1. Matter transport is driven by concentration gradient. Flux (matter) = J m = D dn dz N = number density of particles

More information

Measuring S using an analytical ultracentrifuge. Moving boundary

Measuring S using an analytical ultracentrifuge. Moving boundary Measuring S using an analytical ultracentrifuge Moving boundary [C] t = 0 t 1 t 2 0 top r bottom 1 dr b r b (t) r b ω 2 = S ln = ω 2 S (t-t dt r b (t o ) o ) r b = boundary position velocity = dr b dt

More information

Ch. 19: The Kinetic Theory of Gases

Ch. 19: The Kinetic Theory of Gases Ch. 19: The Kinetic Theory of Gases In this chapter we consider the physics of gases. If the atoms or molecules that make up a gas collide with the walls of their container, they exert a pressure p on

More information

Molecular spectroscopy

Molecular spectroscopy Molecular spectroscopy Origin of spectral lines = absorption, emission and scattering of a photon when the energy of a molecule changes: rad( ) M M * rad( ' ) ' v' 0 0 absorption( ) emission ( ) scattering

More information

Chapter 15 Thermal Properties of Matter

Chapter 15 Thermal Properties of Matter Chapter 15 Thermal Properties of Matter To understand the mole and Avogadro's number. To understand equations of state. To study the kinetic theory of ideal gas. To understand heat capacity. To learn and

More information

Lecture 3: Light absorbance

Lecture 3: Light absorbance Lecture 3: Light absorbance Perturbation Response 1 Light in Chemistry Light Response 0-3 Absorbance spectrum of benzene 2 Absorption Visible Light in Chemistry S 2 S 1 Fluorescence http://www.microscopyu.com

More information

Homework Due by 5PM September 20 (next class) Does everyone have a topic that has been approved by the faculty?

Homework Due by 5PM September 20 (next class) Does everyone have a topic that has been approved by the faculty? Howdy Folks. Homework Due by 5PM September 20 (next class) 5-Problems Every Week due 1 week later. Does everyone have a topic that has been approved by the faculty? Practice your presentation as I will

More information

By: Ashley and Christine Phy 200 Professor Newman 4/13/12

By: Ashley and Christine Phy 200 Professor Newman 4/13/12 By: Ashley and Christine Phy 200 Professor Newman 4/13/12 What is it? Technique used to settle particles in solution against the barrier using centrifugal acceleration Two Types of Centrifuges Analytical

More information

Transport Properties: Momentum Transport, Viscosity

Transport Properties: Momentum Transport, Viscosity Transport Properties: Momentum Transport, Viscosity 13th February 2011 1 Introduction Much as mass(material) is transported within luids (gases and liquids), linear momentum is also associated with transport,

More information

0. Introduction 0.1 Concept The air / environment (geosphere): Is it a reactor? It s a matter of reactions and transports and mixing!

0. Introduction 0.1 Concept The air / environment (geosphere): Is it a reactor? It s a matter of reactions and transports and mixing! 0. Introduction 0.1 Concept The air / environment (geosphere): Is it a reactor? It s a matter of reactions and transports and mixing! mixing times: vertically lower few kilometers (boundary layer) 1h-1d,

More information

Fundamentals of Mass Transfer

Fundamentals of Mass Transfer 1 Fundamentals of Mass Transfer What is mass transfer? When a system contains two or more components whose concentrations vary from point to point, there is a natural tendency for mass to be transferred,

More information

8.6 Drag Forces in Fluids

8.6 Drag Forces in Fluids 86 Drag Forces in Fluids When a solid object moves through a fluid it will experience a resistive force, called the drag force, opposing its motion The fluid may be a liquid or a gas This force is a very

More information

Transport (kinetic) phenomena: diffusion, electric conductivity, viscosity, heat conduction...

Transport (kinetic) phenomena: diffusion, electric conductivity, viscosity, heat conduction... Transport phenomena 1/16 Transport (kinetic) phenomena: diffusion, electric conductivity, viscosity, heat conduction... Flux of mass, charge, momentum, heat,...... J = amount (of quantity) transported

More information

1.3 Molecular Level Presentation

1.3 Molecular Level Presentation 1.3.1 Introduction A molecule is the smallest chemical unit of a substance that is capable of stable, independent existence. Not all substances are composed of molecules. Some substances are composed of

More information

A Fluorometric Analysis of Quinine in Tonic Water

A Fluorometric Analysis of Quinine in Tonic Water A Fluorometric Analysis of Quinine in Tonic Water Introduction In this Laboratory Exercise, we will determine the amount of quinine in Tonic Water using a fluorometric analysis. Fluorescence Spectroscopy

More information

PV = n R T = N k T. Measured from Vacuum = 0 Gauge Pressure = Vacuum - Atmospheric Atmospheric = 14.7 lbs/sq in = 10 5 N/m

PV = n R T = N k T. Measured from Vacuum = 0 Gauge Pressure = Vacuum - Atmospheric Atmospheric = 14.7 lbs/sq in = 10 5 N/m PV = n R T = N k T P is the Absolute pressure Measured from Vacuum = 0 Gauge Pressure = Vacuum - Atmospheric Atmospheric = 14.7 lbs/sq in = 10 5 N/m V is the volume of the system in m 3 often the system

More information

Fluorescence 2009 update

Fluorescence 2009 update XV 74 Fluorescence 2009 update Jablonski diagram Where does the energy go? Can be viewed like multistep kinetic pathway 1) Excite system through A Absorbance S 0 S n Excite from ground excited singlet

More information

LAB #3: FLUROESCENCE SPECTROSCOPY AND ELECTRON TRANSFER (This lab is adapted from the U of MN Phsyical Chemistry lab manual)

LAB #3: FLUROESCENCE SPECTROSCOPY AND ELECTRON TRANSFER (This lab is adapted from the U of MN Phsyical Chemistry lab manual) Chemistry 372 Gustavus Adolphus College A. Purpose LAB #3: FLUROESCENCE SPECTROSCOPY AND ELECTRON TRANSFER (This lab is adapted from the U of MN Phsyical Chemistry lab manual) In this experiment, you will

More information

Chemistry 431. Lecture 1. Introduction Statistical Averaging Electromagnetic Spectrum Black body Radiation. NC State University

Chemistry 431. Lecture 1. Introduction Statistical Averaging Electromagnetic Spectrum Black body Radiation. NC State University Chemistry 431 Lecture 1 Introduction Statistical Averaging Electromagnetic Spectrum Black body Radiation NC State University Overview Quantum Mechanics Failure of classical physics Wave equation Rotational,

More information

Biomolecular hydrodynamics

Biomolecular hydrodynamics Biomolecular hydrodynamics Chem 341, Fall, 2014 1 Frictional coefficients Consider a particle moving with velocity v under the influence of some external force F (say a graviational or electrostatic external

More information

ATM 507 Lecture 4. Text reading Chapters 3 and 4 Today s topics Chemistry, Radiation and Photochemistry review. Problem Set 1: due Sept.

ATM 507 Lecture 4. Text reading Chapters 3 and 4 Today s topics Chemistry, Radiation and Photochemistry review. Problem Set 1: due Sept. ATM 507 Lecture 4 Text reading Chapters 3 and 4 Today s topics Chemistry, Radiation and Photochemistry review Problem Set 1: due Sept. 11 Temperature Dependence of Rate Constants Reaction rates change

More information

Lecture 18 Molecular Motion and Kinetic Energy

Lecture 18 Molecular Motion and Kinetic Energy Physical Principles in Biology Biology 3550 Fall 2017 Lecture 18 Molecular Motion and Kinetic Energy Monday, 2 October c David P. Goldenberg University of Utah goldenberg@biology.utah.edu Fick s First

More information

Hydrodynamic Electrodes and Microelectrodes

Hydrodynamic Electrodes and Microelectrodes CHEM465/865, 2004-3, Lecture 20, 27 th Sep., 2004 Hydrodynamic Electrodes and Microelectrodes So far we have been considering processes at planar electrodes. We have focused on the interplay of diffusion

More information

Brownian Motion and The Atomic Theory

Brownian Motion and The Atomic Theory Brownian Motion and The Atomic Theory Albert Einstein Annus Mirabilis Centenary Lecture Simeon Hellerman Institute for Advanced Study, 5/20/2005 Founders Day 1 1. What phenomenon did Einstein explain?

More information

Kinetic theory. Collective behaviour of large systems Statistical basis for the ideal gas equation Deviations from ideality

Kinetic theory. Collective behaviour of large systems Statistical basis for the ideal gas equation Deviations from ideality Kinetic theory Collective behaviour of large systems Statistical basis for the ideal gas equation Deviations from ideality Learning objectives Describe physical basis for the kinetic theory of gases Describe

More information

Kinetics. Rate of change in response to thermodynamic forces

Kinetics. Rate of change in response to thermodynamic forces Kinetics Rate of change in response to thermodynamic forces Deviation from local equilibrium continuous change T heat flow temperature changes µ atom flow composition changes Deviation from global equilibrium

More information

Lecture 27. Transition States and Enzyme Catalysis

Lecture 27. Transition States and Enzyme Catalysis Lecture 27 Transition States and Enzyme Catalysis Reading for Today: Chapter 15 sections B and C Chapter 16 next two lectures 4/8/16 1 Pop Question 9 Binding data for your thesis protein (YTP), binding

More information

KINETIC THEORY OF GASES

KINETIC THEORY OF GASES KINETIC THEORY OF GASES VERY SHORT ANSWER TYPE QUESTIONS ( MARK). Write two condition when real gases obey the ideal gas equation ( nrt). n number of mole.. If the number of molecule in a container is

More information

Chapter 14. The Ideal Gas Law and Kinetic Theory

Chapter 14. The Ideal Gas Law and Kinetic Theory Chapter 14 The Ideal Gas Law and Kinetic Theory 14.1 Molecular Mass, the Mole, and Avogadro s Number The atomic number of an element is the # of protons in its nucleus. Isotopes of an element have different

More information

Chapter 13 Lecture Lecture Presentation. Chapter 13. Chemical Kinetics. Sherril Soman Grand Valley State University Pearson Education, Inc.

Chapter 13 Lecture Lecture Presentation. Chapter 13. Chemical Kinetics. Sherril Soman Grand Valley State University Pearson Education, Inc. Chapter 13 Lecture Lecture Presentation Chapter 13 Chemical Kinetics Sherril Soman Grand Valley State University Ectotherms Lizards, and other cold-blooded creatures, are ectotherms animals whose body

More information

An Introduction to Diffraction and Scattering. School of Chemistry The University of Sydney

An Introduction to Diffraction and Scattering. School of Chemistry The University of Sydney An Introduction to Diffraction and Scattering Brendan J. Kennedy School of Chemistry The University of Sydney 1) Strong forces 2) Weak forces Types of Forces 3) Electromagnetic forces 4) Gravity Types

More information

Physics of biological membranes, diffusion, osmosis Dr. László Nagy

Physics of biological membranes, diffusion, osmosis Dr. László Nagy Physics of biological membranes, diffusion, osmosis Dr. László Nagy -Metabolic processes and transport processes. - Macrotransport : transport of large amount of material : through vessel systems : in

More information

T(K) k(cm 3 /molecule s) 7.37 x x x x x 10-12

T(K) k(cm 3 /molecule s) 7.37 x x x x x 10-12 CHM 5423 Atmospheric Chemistry Problem Set 3 Due date: Tuesday, February 19 th. The first hour exam is on Thursday, February 21 st. It will cover material from the first four handouts for the class. Do

More information

Luminescence. Photoluminescence (PL) is luminescence that results from optically exciting a sample.

Luminescence. Photoluminescence (PL) is luminescence that results from optically exciting a sample. Luminescence Topics Radiative transitions between electronic states Absorption and Light emission (spontaneous, stimulated) Excitons (singlets and triplets) Franck-Condon shift(stokes shift) and vibrational

More information

Introduction to Spectroscopic methods

Introduction to Spectroscopic methods Introduction to Spectroscopic methods Spectroscopy: Study of interaction between light* and matter. Spectrometry: Implies a quantitative measurement of intensity. * More generally speaking electromagnetic

More information

Correlation Spectroscopy in Polymer Physics Methodenseminar im Wahlpflichtfach Basics diffusion and brownian motion correlations functions

Correlation Spectroscopy in Polymer Physics Methodenseminar im Wahlpflichtfach Basics diffusion and brownian motion correlations functions Correlation Spectroscopy in Polymer Physics Methodenseminar im Wahlpflichtfach 3 1. Basics diffusion and brownian motion correlations functions 2. Dynamic light scattering (DLS) DLS on cellulose solutions

More information

Chapter 17: Fundamentals of Spectrophotometry

Chapter 17: Fundamentals of Spectrophotometry Chapter 17: Fundamentals of Spectrophotometry Spectroscopy: the science that deals with interactions of matter with electromagnetic radiation or other forms energy acoustic waves, beams of particles such

More information

SC/BIOL Current Topics in Biophysics TERM TEST ONE

SC/BIOL Current Topics in Biophysics TERM TEST ONE Page 1 of 1 SC/BIOL 2090.02 Current Topics in Biophysics TERM TEST ONE Name: KEY Student ID: There are three questions. You must complete all three. Ensure that you show your work (that is, equations,

More information

Aula 5 e 6 Transferência de Energia e Transferência de Elétron Caminhos de espécies fotoexcitadas

Aula 5 e 6 Transferência de Energia e Transferência de Elétron Caminhos de espécies fotoexcitadas Fotoquímica Aula 5 e 6 Transferência de Energia e Transferência de Elétron Prof. Amilcar Machulek Junior IQ/USP - CEPEMA Caminhos de espécies fotoexcitadas 1 Diagrama de Jablonski S 2 Relaxation (τ < 1ps)

More information

University of Washington Department of Chemistry Chemistry 453 Winter Quarter 2005

University of Washington Department of Chemistry Chemistry 453 Winter Quarter 2005 Lecture /4/ University of Washington Department of Chemistry Chemistry 4 Winter Quarter A. Polymer Properties of DNA When a linear polymer like DNA becomes long enough it can no longer be treated as a

More information

(2) The volume of molecules is negligible in comparison to the volume of gas. (3) Molecules of a gas moves randomly in all direction.

(2) The volume of molecules is negligible in comparison to the volume of gas. (3) Molecules of a gas moves randomly in all direction. 9.1 Kinetic Theory of Gases : Assumption (1) The molecules of a gas are identical, spherical and perfectly elastic point masses. (2) The volume of molecules is negligible in comparison to the volume of

More information

Chapter 3 Energy Balance and Temperature. Astro 9601

Chapter 3 Energy Balance and Temperature. Astro 9601 Chapter 3 Energy Balance and Temperature Astro 9601 1 Topics to be covered Energy Balance and Temperature (3.1) - All Conduction (3..1), Radiation (3.. and 3...1) Convection (3..3), Hydrostatic Equilibrium

More information

chemical reactions two basic questions: 1) What is the driving force behind a chemical reaction? 2) How fast does a chemical reaction proceed?

chemical reactions two basic questions: 1) What is the driving force behind a chemical reaction? 2) How fast does a chemical reaction proceed? chemical reactions two basic questions: + + 1) What is the driving force behind a chemical reaction? 2) How fast does a chemical reaction proceed? Chemical thermodynamics - What drives a chemical reaction?

More information

Wavelength λ Velocity v. Electric Field Strength Amplitude A. Time t or Distance x time for 1 λ to pass fixed point. # of λ passing per s ν= 1 p

Wavelength λ Velocity v. Electric Field Strength Amplitude A. Time t or Distance x time for 1 λ to pass fixed point. # of λ passing per s ν= 1 p Introduction to Spectroscopy (Chapter 6) Electromagnetic radiation (wave) description: Wavelength λ Velocity v Electric Field Strength 0 Amplitude A Time t or Distance x Period p Frequency ν time for 1

More information

This is a statistical treatment of the large ensemble of molecules that make up a gas. We had expressed the ideal gas law as: pv = nrt (1)

This is a statistical treatment of the large ensemble of molecules that make up a gas. We had expressed the ideal gas law as: pv = nrt (1) 1. Kinetic Theory of Gases This is a statistical treatment of the large ensemble of molecules that make up a gas. We had expressed the ideal gas law as: pv = nrt (1) where n is the number of moles. We

More information

Chemistry 25 (Spring term 2016) Final Examination for NON-SENIORS GOOD LUCK AND HAVE A GREAT SUMMER!!!

Chemistry 25 (Spring term 2016) Final Examination for NON-SENIORS GOOD LUCK AND HAVE A GREAT SUMMER!!! Name ANSWER KEY Distributed Thursday, June 2 Due Chemistry 25 (Spring term 2016) Final Examination for NON-SENIORS GOOD LUCK AND HAVE A GREAT SUMMER!!! by Thursday, June 2 at 1 pm to 362 Broad a drop box

More information

Reflection = EM strikes a boundary between two media differing in η and bounces back

Reflection = EM strikes a boundary between two media differing in η and bounces back Reflection = EM strikes a boundary between two media differing in η and bounces back Incident ray θ 1 θ 2 Reflected ray Medium 1 (air) η = 1.00 Medium 2 (glass) η = 1.50 Specular reflection = situation

More information

If the position of a molecule is measured after increments of 10, 100, 1000 steps, what will the distribution of measured steps look like?

If the position of a molecule is measured after increments of 10, 100, 1000 steps, what will the distribution of measured steps look like? If the position of a molecule is measured after increments of 10, 100, 1000 steps, what will the distribution of measured steps look like? (1) No longer Gaussian (2) Identical Gaussians (3) Gaussians with

More information

Homework: 13, 14, 18, 20, 24 (p )

Homework: 13, 14, 18, 20, 24 (p ) Homework: 13, 14, 18, 0, 4 (p. 531-53) 13. A sample of an ideal gas is taken through the cyclic process abca shown in the figure below; at point a, T=00 K. (a) How many moles of gas are in the sample?

More information

Experimental Design and Data Collection

Experimental Design and Data Collection A. Checks to run to make sure the instrument is in good working condition B. Decide which experiment type is most appropriate, equilibrium or velocity C. Buffer considerations D. Speed selection and length

More information

Chemical Processes. Transport Processes in the Environment. Transport Processes. Advection. Advection. t 1 t 2

Chemical Processes. Transport Processes in the Environment. Transport Processes. Advection. Advection. t 1 t 2 hemical Processes by Stefan Trapp (taken from course 4) Transport Processes in the Environment a definition of our nomenklatura Transport Processes Only 3 types of transport processes exist ) by advection

More information

Convective Mass Transfer

Convective Mass Transfer Convective Mass Transfer Definition of convective mass transfer: The transport of material between a boundary surface and a moving fluid or between two immiscible moving fluids separated by a mobile interface

More information

Physics Assessment Unit A2 2

Physics Assessment Unit A2 2 Centre Number 71 Candidate Number ADVANCED General Certificate of Education 2014 Physics Assessment Unit A2 2 assessing Fields and their Applications AY221 [AY221] MONDAY 9 JUNE, MORNING TIME 1 hour 30

More information

Appendix 1: List of symbols

Appendix 1: List of symbols Appendix 1: List of symbols Symbol Description MKS Units a Acceleration m/s 2 a 0 Bohr radius m A Area m 2 A* Richardson constant m/s A C Collector area m 2 A E Emitter area m 2 b Bimolecular recombination

More information

Carriers Concentration and Current in Semiconductors

Carriers Concentration and Current in Semiconductors Carriers Concentration and Current in Semiconductors Carrier Transport Two driving forces for carrier transport: electric field and spatial variation of the carrier concentration. Both driving forces lead

More information

Discussion Session prior to the Second Examination: Sunday evening April 13 6 to 8 pm. 161 Noyes Laboratory

Discussion Session prior to the Second Examination: Sunday evening April 13 6 to 8 pm. 161 Noyes Laboratory Discussion Session prior to the Second Examination: Sunday evening April 13 6 to 8 pm 161 Noyes Laboratory Determination of the Stokes Radius by measuring the Rotational Diffusion Coefficient: D rot D

More information

BCIT Fall Chem Exam #1

BCIT Fall Chem Exam #1 BCIT Fall 2012 Chem 3615 Exam #1 Name: Attempt all questions in this exam. Read each question carefully and give a complete answer in the space provided. Part marks given for wrong answers with partially

More information

Radiative Transfer Chapter 3, Hartmann

Radiative Transfer Chapter 3, Hartmann Radiative Transfer Chapter 3, Hartmann Shortwave Absorption: Clouds, H 2 0, O 3, some CO 2 Shortwave Reflection: Clouds, surface, atmosphere Longwave Absorption: Clouds, H 2 0, CO 2, CH 4, N 2 O Planck

More information

Lecture 7: Enzymes and Energetics

Lecture 7: Enzymes and Energetics Lecture 7: Enzymes and Energetics I. Biological Background A. Biological work requires energy 1. Energy is the capacity to do work a. Energy is expressed in units of work (kilojoules) or heat energy (kilocalories)

More information

Chapter 3 Energy Balance and Temperature. Topics to be covered

Chapter 3 Energy Balance and Temperature. Topics to be covered Chapter 3 Energy Balance and Temperature Astro 9601 1 Topics to be covered Energy Balance and Temperature (3.1) - All Conduction (3..1), Radiation (3.. and31) 3...1) Convection (3..3), Hydrostatic Equilibrium

More information

Chapter 17: Fundamentals of Spectrophotometry

Chapter 17: Fundamentals of Spectrophotometry Chapter 17: Fundamentals of Spectrophotometry Spectroscopy: the science that deals with interactions of matter with electromagnetic radiation or other forms energy acoustic waves, beams of particles such

More information

1. Strahlungsgesetze, Ableitung der Planck-schen Strahlungsformel, Einstein-Koeffizienten, Extinktinskoeffizient, Oszillatorenstärke

1. Strahlungsgesetze, Ableitung der Planck-schen Strahlungsformel, Einstein-Koeffizienten, Extinktinskoeffizient, Oszillatorenstärke 1. Strahlungsgesetze, Ableitung der Planck-schen Strahlungsformel, Einstein-Koeffizienten, Extinktinskoeffizient, Oszillatorenstärke Einheiten in diesem Kapitel: diesmal cgs. Energy volume density of blackbody

More information

Handout 11: Ideal gas, internal energy, work and heat. Ideal gas law

Handout 11: Ideal gas, internal energy, work and heat. Ideal gas law Handout : Ideal gas, internal energy, work and heat Ideal gas law For a gas at pressure p, volume V and absolute temperature T, ideal gas law states that pv = nrt, where n is the number of moles and R

More information

L = I ω = const. I = 2 3 MR2. When the balloon shrinks (because the air inside it cools down), the moment of inertia decreases, R = 1. L = I ω = I ω.

L = I ω = const. I = 2 3 MR2. When the balloon shrinks (because the air inside it cools down), the moment of inertia decreases, R = 1. L = I ω = I ω. PHY 30 K. Solutions for mid-term test #3. Problem 1: Out in space, there are no forces acting on the balloon except gravity and hence no torques (with respect to an axis through the center of mass). Consequently,

More information